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Remark on non-contractible closed geodesics
and homotopy groups

Egor Shelukhin [email protected] Department of Mathematics and Statistics, University of Montreal, C.P. 6128 Succ. Centre-Ville Montreal, QC H3C 3J7, Canada  and  Jun Zhang [email protected] The Institute of Geometry and Physics, University of Science and Technology of China, 96 Jinzhai Road, Hefei Anhui, 230026, China
Abstract.

We prove that if the mm-th homotopy group for m2m\geq 2 of a closed manifold has non-trivial invariants or coinvariants under the action of the fundamental group, then there exist infinitely many geometrically distinct closed geodesics for a C4C^{4}-generic Riemannian metric. If moreover there are infinitely many conjugacy classes in the fundamental group, then the same holds for every Riemannian metric.

1. Introduction and main results

1.1. Introduction

The question of the existence of infinitely many geometrically distinct closed (periodic) geodesics on Riemannian or Finsler manifolds was studied extensively in the past. This question seeks to determine whether or not for every metric or for a class of metrics on a given manifold MM there exist infinitely many prime closed geodesics: those closed geodesics that are not obtained as iterations of others.

The efforts were primarily focused on the simply-connected case, where by [14, 32, 18] a manifold with finitely many prime closed geodesics must have 𝕂{\mathbb{K}}-cohomology, for 𝕂={\mathbb{K}}={\mathbb{Q}} or 𝕂=𝔽p,{\mathbb{K}}=\mathbb{F}_{p}, generated as a unital 𝕂{\mathbb{K}}-algebra by a single element. Manifolds satisfying this condition for some 𝕂{\mathbb{K}} do exist: notable examples are the compact rank-one symmetric spaces (CROSS): Sn,Pn,Pn,Pn,𝕆P2S^{n},{\mathbb{C}}P^{n},{\mathbb{R}}P^{n},{\mathbb{H}}P^{n},{\mathbb{O}}P^{2}. For such spaces it is known [25] that a C2C^{2}-generic metric must have infinitely many prime closed geodesics. Prior work [19, 16] proves the same for C4C^{4}-generic metrics: [19] implies that C4C^{4}-generically on any closed manifold there are infinitely many prime closed geodesics, unless they are all hyperbolic, while [16] proves that for manifolds rationally homotopy equivalent to a CROSS other than Pn,{\mathbb{R}}P^{n}, given that all prime closed geodesics are hyperbolic, there are infinitely many of them. The case of Pn{\mathbb{R}}P^{n} follows by a quick covering argument, as does the case of any closed manifold with finite fundamental group, or by the paper [4] discussed below. A celebrated result [5, 12, 17] proves that every Riemannian metric on S2S^{2} has infinitely many prime closed geodesics, and the same is true for P2{\mathbb{R}}P^{2}. The analogous statement for any other CROSS is a well-known open question.

The case of infinite fundamental groups at first appears to be simpler, as by a classical theorem often attributed to Cartan or to Hilbert (see for example [11, Chapter 12, Theorem 2.2]), in every non-trivial free homotopy class of loops on MM there exists a closed geodesic. However, firstly, it is an open question in group theory [22, 8] whether an infinite finitely presented group could have finitely many conjugacy classes. We recall that the conjugacy classes in π1(M)\pi_{1}(M) correspond to free homotopy classes of loops on MM. Secondly, even if we assume that there are infinitely many conjugacy classes, the simplification appears to be quite illusory, starting with the fact that non-homotopic closed geodesics might not be geometrically distinct (see also [29]). Existence of infinitely many prime closed geodesics is currently known under stronger conditions involving the fundamental group: for example [6] if the manifold is not the circle and its fundamental group is {\mathbb{Z}} (see [30, 31, 26] for other conditions of this kind and [15, 3] for prior work). Generic existence (in C4C^{4} topology) of infinitely many prime closed geodesics was proved under special conditions on π1(M)\pi_{1}(M) in [4]: for instance this covers the case where π1(M)\pi_{1}(M) has finitely many conjugacy classes, yet is not simply-connected. The recent work [26] proves C4C^{4}-generic existence of infinitely many prime closed geodesics on every closed 33-manifold, and produces further results about closed geodesics on connected sums of closed manifolds (see also [23, 21]).

Our main result shows that C4C^{4}-generic existence of infinitely many prime closed geodesics holds on closed manifolds, of any dimension, under a topological condition regarding the action of π1(M)\pi_{1}(M) on πm(M)\pi_{m}(M) for m2,m\geq 2, in the spirit of Bangert-Hingston [6], Albers-Frauenfelder-Oancea [1] and Taimanov [30], which have inspired this paper. Namely, we assume that this action for some m2m\geq 2 has either non-trivial invariants or non-trivial coinvariants. We also prove that if in addition there are infinitely many free homotopy classes of loops on M,M, then there exist infinitely many prime closed geodesics for every Riemannian metric on M.M.

1.2. Main results

Theorem A.

Let MM be a closed manifold. Suppose that there exists xπm(M),x\in\pi_{m}(M), x0,x\neq 0, for m2m\geq 2 such that ax=xa\cdot x=x for all aπ1(M)a\in\pi_{1}(M) or a homomorphism ξ:πm(M)A,\xi:\pi_{m}(M)\to A, ξ0\xi\neq 0 to an abelian group AA such that aξ=ξa^{*}\xi=\xi for all aπ1(M).a\in\pi_{1}(M). Moreover, let the set π1(M)/conj\pi_{1}(M)/{\mathrm{conj}} of conjugacy classes in π1(M)\pi_{1}(M) be infinite. Then for every Riemannian metric on MM there exist infinitely many geometrically distinct closed geodesics.

Remark 1.

We remark that our condition on the higher homotopy groups does not constrain the fundamental group of the manifold. For instance, taking a product with the two-sphere does not change the fundamental group but ensures that this condition holds (see also Remark 5). The condition on coinvariants for m=2m=2 and A=GL(1,𝔽p)A=GL(1,\mathbb{F}_{p}) for a finite field 𝔽p\mathbb{F}_{p} is satisfied if and only if there exists a non-trivial rank-one 𝔽p\mathbb{F}_{p}-local system on M{\mathcal{L}}M with a trivial restriction to MM via the constant loop embedding MM.M\to{\mathcal{L}}M. We refer to [1, Section 2.2] for a related discussion and [1, Proposition 9], showing that this condition, for a suitable prime p,p, is in turn implied by the non-triviality of the image H2S(M;)H_{2}^{S}(M;{\mathbb{Z}}) of the second Hurewicz map π2(M)H2(M;).\pi_{2}(M)\to H_{2}(M;{\mathbb{Z}}).

Recall that the natural map π1(M)π0(M)\pi_{1}(M)\to\pi_{0}({\mathcal{L}}M) from the fundamental group of MM to the set π0(M)\pi_{0}({\mathcal{L}}M) of connected components of the free loop space M{\mathcal{L}}M of MM induces a canonical isomorphism of sets

π1(M)/conjπ0(M),\pi_{1}(M)/{\mathrm{conj}}\xrightarrow{\cong}\pi_{0}({\mathcal{L}}M),

where π1(M)/conj\pi_{1}(M)/{\mathrm{conj}} is the set of conjugacy classes in π1(M).\pi_{1}(M). Hence requiring that the set π1(M)/conj\pi_{1}(M)/{\mathrm{conj}} is infinite is the least possible assumption on the richness of the fundamental group that would help establishing the existence of infinitely many geometrically distinct closed geodesics. In fact, a well-known open question in group theory, due to Makowsky [22] (see also [8]), is whether every infinite finitely-presented group has infinitely many conjugacy classes. Note that the assumption on the conjugacy classes yields infinitely many non-homotopic closed geodesics, as by Cartan and Hilbert’s theorem, there is a closed geodesic in every non-trivial free homotopy class α\alpha of loops on M.M. (It is given as point of global minimum of energy in the corresponding connected component αM{\mathcal{L}}_{\alpha}M of M{\mathcal{L}}M.) However, these geodesics might easily not all be geometrically distinct since a geodesic cc and its kk-th iterate ck,c^{k}, given by ck(t)=c(kt),c^{k}(t)=c(kt), could contribute to different free homotopy classes. In general, the free homotopy class [ck]π0(M)[c^{k}]\in\pi_{0}({\mathcal{L}}M) of the iterate ckc^{k} might depend on kk in a complicated way.

Corollary 2.

Let MM be a closed manifold. Suppose that there exists xπm(M),x\in\pi_{m}(M), x0,x\neq 0, for m2m\geq 2 such that ax=xa\cdot x=x for all aπ1(M)a\in\pi_{1}(M) or a homomorphism ξ:πm(M)A,\xi:\pi_{m}(M)\to A, ξ0\xi\neq 0 to an abelian group AA such that aξ=ξa^{*}\xi=\xi for all aπ1(M).a\in\pi_{1}(M). Then for a C4C^{4}-generic Riemannian metric on MM there exist infinitely many geometrically distinct closed geodesics.

We remark that in this corollary we make no assumption on conjugacy classes in the fundamental group. It appears to be new even for manifolds of the form M=X×S2,M=X\times S^{2}, where XX is an arbitrary closed manifold (see also Remark 5). Of course XX for which prior methods do not apply are more restricted; for instance there should be an element απ1(X)/conj\alpha\in\pi_{1}(X)/{\mathrm{conj}} such that αk,\alpha^{k}, k1,k\geq 1, are all distinct.

Proof of Corollary 2.

If MM is simply connected, the conclusion is well-known by the work of Klingenberg-Takens [19], Hingston [16], and Rademacher [25]. If MM is not simply connected, consider a non-trivial class aπ1(M).a\in\pi_{1}(M). Then either there exist two equal conjugacy classes [ak]=[al][a^{k}]=[a^{l}] for some positive integers 0<k<l,0<k<l, in which case the conclusion follows by work of Ballmann-Thorbergsson-Ziller [4, Theorem A], or the conjugacy classes [ak],[a^{k}], for kk a positive integer, are all distinct, in which case the conclusion follows by Theorem A. ∎

Remark 3.

By the arguments proving [10, Corollary B], one can upgrade Corollary 2 to the stronger conclusion that for C4C^{4}-generic metrics, the number of prime periodic orbits of length at most TT grows exponentially in T.T. (Note that while this is not stated explicitly, [10, Corollary B] is proven therein for simply-connected manifolds.)

Remark 4.

It is not hard to see that Theorem A and Corollary 2 extend to Finsler metrics (the latter in the C6C^{6}-generic case), by a finite-dimensional approximation approach (see [24] as well as [26, 27]). In forthcoming work [28] we will show that an analogue of Corollary 2 holds also for Reeb flows of arbitrary contact forms on the unit cotangent bundle SM,S^{*}M, by proving a weaker analogue of Theorem A. In future work we hope to prove a more direct analogue of Theorem A in the context of Reeb flows.

Remark 5.

It is easy to see that the family 𝒩{\mathcal{N}} of manifolds satisfying the condition of Corollary 2 is an ideal in the family {\mathcal{M}} of all closed manifolds with respect to the Cartesian product. In certain situations, this property is also preserved under connected sums. For instance, consider the family 2{\mathcal{H}}_{2}\subset{\mathcal{M}} of all closed manifolds MM satisfying H2S(M;)0H_{2}^{S}(M;{\mathbb{Z}})\neq 0 (see Remark 1). Set 2m=2m,{\mathcal{H}}^{\geq m}_{2}={\mathcal{H}}_{2}\cap{\mathcal{M}}^{\geq m}, where m{\mathcal{M}}^{\geq m}\subset{\mathcal{M}} is the subfamily of manifolds of dimension at least m.m. Let m=3.m=3. Then 23{\mathcal{H}}^{\geq 3}_{2} is an ideal in 3{\mathcal{M}}^{\geq 3} with respect to connect sum: if X3X\in{\mathcal{M}}^{\geq 3} and Y23Y\in{\mathcal{H}}^{\geq 3}_{2} then X#Y23.X\#Y\in{\mathcal{H}}^{\geq 3}_{2}. This is a consequence of the fact that for manifolds X,Y3,X,Y\in{\mathcal{M}}^{\geq 3}, by the homotopy exact sequence of a pair, π2(X#Y)π2(X)π2(Y),\pi_{2}(X\#Y)\cong\pi_{2}(X)\oplus\pi_{2}(Y), and the Mayer-Vietoris sequence for the natural covering XY=X#Y,X^{\prime}\cup Y^{\prime}=X\#Y, where XXBX,YYBYX^{\prime}\cong X\setminus B_{X},Y^{\prime}\cong Y\setminus B_{Y} for closed balls BXX,BYY.B_{X}\subset X,B_{Y}\subset Y. In all dimensions nn other than n{0,1,3}n\in\{0,1,3\} there exist simply-connected manifolds Xn2X^{n}\in{\mathcal{H}}_{2} of dimension n.n. Indeed, for n=2,n=2, X2=S2X^{2}=S^{2} and for n4,n\geq 4, we can take Xn=S2×Sn2.X^{n}=S^{2}\times S^{n-2}. Combining with the previous point, we see by the Van Kampen theorem, that for every manifold M4M\in{\mathcal{M}}^{\geq 4} there exists a manifold M24M^{\prime}\in{\mathcal{H}}^{\geq 4}_{2} with π1(M)π1(M).\pi_{1}(M^{\prime})\cong\pi_{1}(M). We can take M=M#Xn.M^{\prime}=M\#X^{n}. Similarly, for all M,M\in{\mathcal{M}}, M′′=M×Xn2M^{\prime\prime}=M\times X^{n}\in{\mathcal{H}}_{2} satisfies π1(M′′)π1(M).\pi_{1}(M^{\prime\prime})\cong\pi_{1}(M).

Remark 6.

One could imagine a generalization of Corollary 2 which would hold for all closed non-aspherical manifolds, and a suitable generalization of Theorem A. However, the complicated algebraic properties of the group rings [π1(M)],{\mathbb{Z}}[\pi_{1}(M)], which are, for instance, often non-Noetherian [20], seem to be an obstruction to proving such results.

2. Preliminaries

2.1. Average index and homotopy groups.

Let (M,g)(M,g) be a Riemannian manifold of dimension dimM=n.\dim M=n. Let ind(c)\operatorname{\mathrm{ind}}(c) denote the index of a closed geodesic cc in (M,g).(M,g). The average index (or mean-index) of cc is defined as

Δ(c)=limmind(cm)m.\Delta(c)=\lim_{m\to\infty}\frac{\operatorname{\mathrm{ind}}(c^{m})}{m}\in{\mathbb{R}}.

It satisfies the following useful properties (see [13, Proposition 6.1, Equation (6.1.3)] and [24, Korollar 4.4] for instance):

  1. (1)

    Δ(cm)=mΔ(c)\Delta(c^{m})=m\Delta(c) for all m>0m\in{\mathbb{Z}}_{>0}

  2. (2)

    |Δ(c)ind(c)|n1,|\Delta(c)-\operatorname{\mathrm{ind}}(c)|\leq n-1, |Δ(c)(ind(c)+null(c))|n1|\Delta(c)-(\operatorname{\mathrm{ind}}(c)+\mathrm{null}(c))|\leq n-1

  3. (3)

    Δ(c)0\Delta(c)\geq 0 and Δ(c)=0\Delta(c)=0 if and only if ind(cm)=0\operatorname{\mathrm{ind}}(c^{m})=0 for all m>0.m\in{\mathbb{Z}}_{>0}.

Let Λα\Lambda_{\alpha} be the L12L^{2}_{1}-completion of αM{\mathcal{L}}_{\alpha}M and ΛαA={𝒜<A}\Lambda_{\alpha}^{A}=\{\mathcal{A}<A\} for A>0.A>0. Note that the inclusion αAMΛαAM{\mathcal{L}}^{A}_{\alpha}M\to\Lambda^{A}_{\alpha}M is a homotopy equivalence for every A>0A>0 by a result of Anosov [2] (see also [13, Proposition 2.2]).

We require the following property of the homotopy groups of ΛαM,\Lambda_{\alpha}M, which follows from [14] and the properties of the mean-index (see also [9]).

Proposition 7.

If all geodesics bΛαMb\in\Lambda_{\alpha}M with 𝒜(b)A\mathcal{A}(b)\geq A are of mean-index Δ(b)>k+n1,\Delta(b)>k+n-1, then πm(Λα)=πm(ΛαA)\pi_{m}(\Lambda_{\alpha})=\pi_{m}(\Lambda_{\alpha}^{A}) for all mk.m\leq k.

We recall the following long exact sequence from [30]. Fix απ0(M).\alpha\in\pi_{0}({\mathcal{L}}M). Consider the evaluation map ev:ΛαMM,ev:\Lambda_{\alpha}M\to M, zz(0),z\mapsto z(0), where zΛαMz\in\Lambda_{\alpha}M is considered as an absolutely continuous map z:/Mz:{\mathbb{R}}/{\mathbb{Z}}\to M with square-integrable velocity vector. This map is a Serre fibration. Fix base-points x0Mx_{0}\in M and γ0ev1(x0).\gamma_{0}\in ev^{-1}(x_{0}). Let aπ1(M,x0)a\in\pi_{1}(M,x_{0}) be the class represented by γ0.\gamma_{0}. Of course [a]=α[a]=\alpha in π1(M)/conj.\pi_{1}(M)/{\mathrm{conj}}.

Proposition 8.

The long exact sequence of a fibration for evev and an identification πk(ev1(x0),γ0)πk+1(M,x0)\pi_{k}(ev^{-1}(x_{0}),\gamma_{0})\cong\pi_{k+1}(M,x_{0}) yield the long exact sequence:

πm+1(M,x0)1aπm+1(M,x0)πm(ΛαM,γ0)πm(M,x0)1aπm(M,x0),\ldots\to\pi_{m+1}(M,x_{0})\xrightarrow{1-a}\pi_{m+1}(M,x_{0})\to\pi_{m}(\Lambda_{\alpha}M,\gamma_{0})\to\pi_{m}(M,x_{0})\xrightarrow{1-a}\pi_{m}(M,x_{0})\to\ldots,

for m2,m\geq 2, where a:πk(M,x0)πk(M,x0)a:\pi_{k}(M,x_{0})\to\pi_{k}(M,x_{0}) is the standard action of the fundamental group on higher homotopy groups. For m=1m=1 the sequence reads:

π2(M,x0)1aπ2(M,x0)π1(ΛαM,γ0)Ca1,\ldots\to\pi_{2}(M,x_{0})\xrightarrow{1-a}\pi_{2}(M,x_{0})\to\pi_{1}(\Lambda_{\alpha}M,\gamma_{0})\to C_{a}\to 1,

where Caπ1(M,x0)C_{a}\subset\pi_{1}(M,x_{0}) is the centralizer of a.a.

3. Proof of main result

Proof of Theorem A.

By Proposition 8, the hypothesis of the theorem implies that π(ΛαM)0\pi_{\ell}(\Lambda_{\alpha}M)\neq 0 for =m\ell=m or =m1\ell=m-1 and all απ0(M).\alpha\in\pi_{0}({\mathcal{L}}M).

Suppose by contradiction that there are finitely many prime closed geodesics. (In particular, every closed geodesic is isolated.) We denote them by γ1,,γP,γP+1,,γN,\gamma_{1},...,\gamma_{P},\gamma_{P+1},...,\gamma_{N}, such that the geodesics γ1,,γP\gamma_{1},...,\gamma_{P} have mean-index Δ(γi)>0\Delta(\gamma_{i})>0 and γi\gamma_{i} for i>Pi>P have Δ(γi)=0.\Delta(\gamma_{i})=0. Then by Property (3) of the mean-index, for every i>P,i>P, ind(γij)=0\operatorname{\mathrm{ind}}(\gamma_{i}^{j})=0 for all iterations j.j. Now all closed geodesics are iterations of γ1,,γN\gamma_{1},\ldots,\gamma_{N}. Consider the set SS of all the conjugacy classes [γij],[\gamma_{i}^{j}], 1iP1\leq i\leq P such that Δ(γij)n1+.\Delta(\gamma_{i}^{j})\leq n-1+\ell. Since the mean-indices of γi\gamma_{i} for 1iP1\leq i\leq P are positive, by Property (1) of the mean-index, SS is a finite set. Since π0(M)\pi_{0}({\mathcal{L}}M) is an infinite set, so is the complement π0(M)S.\pi_{0}({\mathcal{L}}M)\setminus S. Consider απ0(M)S.\alpha\in\pi_{0}({\mathcal{L}}M)\setminus S. Now let c1,,crΛαMc_{1},\ldots,c_{r}\in\Lambda_{\alpha}M be all the points of absolute minimum of the energy functional on ΛαM\Lambda_{\alpha}M. Then the level set of this minimum is the disjoint union j=1rS(cj)),\sqcup_{j=1}^{r}S(c_{j})), where S(cj)S(c_{j}) is the circle given by cjc_{j} and its rotations, and therefore its kk-th homotopy groups vanish for all k>1.k>1. We now claim that there exists a geodesic ηΛαM\eta\in\Lambda_{\alpha}M that is not a global minimum and is not an iteration of any of γ1,,γP.\gamma_{1},...,\gamma_{P}. Note that as η\eta must be an iteration of some γi\gamma_{i} for i>Pi>P we must have ind(ηr)=0\operatorname{\mathrm{ind}}(\eta^{r})=0 for all r1.r\geq 1. By Bangert-Klingenberg [7, Theorem 3], this implies that there exist infinitely many prime closed geodesics on M.M.

To prove the last claim, we treat the cases 2\ell\geq 2 and =1\ell=1 slightly differently. Suppose first that 2.\ell\geq 2. The contrapositive assumption that all closed geodesics above the minimum energy are iterations of γ1,,γP\gamma_{1},\ldots,\gamma_{P}, implies that π(ΛαM)=0\pi_{\ell}(\Lambda_{\alpha}M)=0 by Proposition 7, since by construction, any iteration η\eta of γ1,,γP\gamma_{1},\ldots,\gamma_{P} in α\alpha has Δ(η)>n1+.\Delta(\eta)>n-1+\ell. But we know that π(ΛαM)0.\pi_{\ell}(\Lambda_{\alpha}M)\neq 0. In the case where =1,\ell=1, we observe that the coinvariant hypothesis and Proposition 8 yields that ker(ev:π1(ΛαM,γ0)π1(M,x0))0.\ker(ev:\pi_{1}(\Lambda_{\alpha}M,\gamma_{0})\to\pi_{1}(M,x_{0}))\neq 0. Now, we argue that there can only be one point of global minimum under the contrapositive assumption. Indeed, had we N>1N>1 global minima c1,,cNc_{1},\ldots,c_{N}, the contrapositive assumption would yield that π0(ΛαM)\pi_{0}(\Lambda_{\alpha}M) is a set of NN elements, which contradicts the connectedness of ΛαM.\Lambda_{\alpha}M. Hence there is a unique global minimum c.c. Now the contrapositive assumption yields that π1(ΛαM)π1(S(c))\pi_{1}(\Lambda_{\alpha}M)\cong\pi_{1}(S(c))\cong{\mathbb{Z}} and the evaluation map π1(S(c))Ca\pi_{1}(S(c))\to C_{a} is injective. This is a contradiction to its kernel being non-zero. This proves the claim for all 1.\ell\geq 1.

Acknowledgements

We thank the participants of the reading group on closed geodesics at the Université de Montréal, especially Marco Mazzucchelli, for useful discussions. E.S. was supported by an NSERC Discovery grant, by the Fonds de recherche du Québec - Nature et technologies, by the Fondation Courtois, and by an Alfred P. Sloan Research Fellowship. This work was partially supported by the National Science Foundation under Grant No. DMS-1928930, while E.S. was in residence at the Simons Laufer Mathematical Sciences Institute (previously known as MSRI) Berkeley, California during the Fall 2022 semester. J.Z. is supported by USTC Research Funds of the Double First-Class Initiative. This work was initiated when J.Z. was a CRM-ISM Postdoctoral Research Fellow at CRM, Université de Montréal, and he thanks this institute for its warm hospitality.

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